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Electronic structure, self-doping, and superconducting instability in the alternating single-layer trilayer stacking nickelates
Yang Zhang, Ling-Fang Lin, Adriana Moreo, Thomas A. Maier, and Elbio Dagotto
Phys. Rev. B 110, L060510 – Published 14 August 2024
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Abstract
Motivated by the recently proposed alternating single-layer trilayer stacking structure for the nickelate , we comprehensively study this system using ab initio and random-phase approximation techniques. Our analysis unveils similarities between this novel structure and other Ruddlesden-Popper nickelate superconductors, such as a similar charge-transfer gap value and orbital-selective behavior of the orbitals. Pressure primarily increases the bandwidths of the Ni bands, suggesting an enhancement of the itinerant properties of those states. By changing the cell volume ratio from 0.9 to 1.10, we found that the bilayer structure in always has lower energy than the single-layer trilayer stacking . In addition, we observe a “self-doping” effect (compared to the average 1.5 electrons per orbital per site of the entire structure) from the trilayer to the single-layer sublattices and this effect will be enhanced by overall electron doping. Moreover, we find a leading -wave pairing state that is restricted to the single layer. Because the effective coupling between the single layers is very weak, due to the nonsuperconducting trilayer in-between, this suggests that the superconducting transition temperature in this structure should be much lower than in the bilayer structure.
- Received 24 April 2024
- Revised 15 July 2024
- Accepted 31 July 2024
DOI:https://doi.org/10.1103/PhysRevB.110.L060510
©2024 American Physical Society
Physics Subject Headings (PhySH)
- Research Areas
Multiband superconductivityPairing mechanismsSuperconductivity
- Physical Systems
High-temperature superconductorsNickelates
- Techniques
Electron-correlation calculationsFirst-principles calculationsHubbard modelRandom phase approximationWannier function methods
Condensed Matter, Materials & Applied Physics
Authors & Affiliations
Yang Zhang1, Ling-Fang Lin1, Adriana Moreo1,2, Thomas A. Maier3, and Elbio Dagotto1,2
- 1Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA
- 2Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
- 3Computational Sciences and Engineering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
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Issue
Vol. 110, Iss. 6 — 1 August 2024
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Article part of CHORUS
Accepted manuscript will be available starting14 August 2025.Images
Figure 1
(a)Schematic crystal structure of the conventional cells of the high-pressure phase of 327-LNO (BL) and phase of 327-LNO (SL-TL), respectively (green = La; gray = Ni; red = O). All crystal structures were visualized using the vesta code [59]. (b)Sketches of electronic states in the BL and SL-TL. The light blue (pink) horizontal lines represent () states. The solid and open circles represent 1.0 and 0.5 electrons, respectively. The total population of electrons considered is and 6.0 electrons, for BL with two sites and SL-TL with four sites, respectively. (c)The Ni orbitals projected band structures and density of states. The and orbitals are distinguished by the blue and red lines. (d)FS for the nonmagnetic state of the high-pressure phase of the 327-LNO (SL-TL) structure at 16GPa. Note that the local axis is perpendicular to the plane towards the top O atom, while the local or axis is along the in-plane Ni-O bond directions.
Figure 2
(a)Calculated energies of different structural phases of 327-LNO (SL-TL) and 327-LNO (BL), as a function of the ratio . Here, is the conventional-cell volume of the phase of 327-LNO (SL-TL) at 16GPa. The phase of 327-LNO (SL-TL) is taken as the energy of reference. (b), (c)The Ni orbitals projected band structure for the (b) and (c) phases, respectively.
Figure 3
(a)Tight-binding band structure and (b)FS for the phase of 327-LNO (SL-TL) at 16GPa. Here, an eight-band -orbital tight-binding model was considered including SL and TL hoppings (see the hopping file in the Supplemental Material [63]) with an overall filling of (i.e., 1.5 electrons per site). (c)Crude sketches of the crystal-field splitting of the orbitals for different Ni sites. All the values are given in units of eV. (d)The total electron occupations and (e) different electronic densities of the orbitals for the different Ni sites vs the overall filling in the tight-binding model. The red line in (d)represents the average electronic Ni site occupancy.
Figure 4
The RPA calculated leading superconducting singlet gap structure for momenta on the FS of 327-LNO (SL-TL) at and their pairing strength : (a)Leading -wave state with , (b)subleading -wave state with , (c)-wave state with . The sign of the gap structure is indicated by the colors (orange = positive, blue = negative), and the gap amplitude by the point size. The RPA calculations used Coulomb interaction parameters (intraorbital), (interorbital), and (Hund coupling and pair hopping, respectively) in units of eV. The hopping parameters are available in the Supplemental Material [63]. The dominant character of the Fermi-surface Bloch states arising from the SL (magenta) and TL (cyan) sublattices is shown in (d).